標(biāo)題: Titlebook: Elements of Quantum Optics; Pierre Meystre,Murray Sargent Textbook 19912nd edition Springer-Verlag Berlin Heidelberg 1991 Absorption.Laser [打印本頁(yè)] 作者: Harrison 時(shí)間: 2025-3-21 18:45
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書(shū)目名稱(chēng)Elements of Quantum Optics讀者反饋
書(shū)目名稱(chēng)Elements of Quantum Optics讀者反饋學(xué)科排名
作者: exigent 時(shí)間: 2025-3-21 20:39 作者: 停止償付 時(shí)間: 2025-3-22 00:47 作者: 確認(rèn) 時(shí)間: 2025-3-22 05:42 作者: 色情 時(shí)間: 2025-3-22 08:43 作者: barium-study 時(shí)間: 2025-3-22 16:36
Brian Milakovsky,Brent Frey,Thomas Jameswhen this approach is justified and what to do when it isn’t. Unexcited systems interacting with radiation far from the system resonances can often be treated purely classically. The response of systems near and at resonance often deviates substantially from the classical descriptions. Since the las作者: barium-study 時(shí)間: 2025-3-22 18:36
The DMZ and the Destiny of a Divided Korea,the equations of motion for the probability amplitudes. However two important kinds cannot upper to lower level decay, and more rapid decay of the electric dipole than the average level decay rate. For these two damping mechanisms, we need a more general description than can be provided by the state作者: MOTTO 時(shí)間: 2025-3-22 21:57 作者: Heterodoxy 時(shí)間: 2025-3-23 05:03
https://doi.org/10.1007/978-3-658-10373-6interaction of radiation with two-level atoms. We consider arrangements of two or three highly reflecting mirrors that form cavities as shown in Fig. 6-1. Light in these cavities leaks out (decays to its 1/. value) in a time ./. where . is the frequency of the light and . is the cavity quality facto作者: 昆蟲(chóng) 時(shí)間: 2025-3-23 05:41 作者: 使隔離 時(shí)間: 2025-3-23 12:20
Schering: Synchronised Drug Developmentility, etc. Alternatively one can use them to study the properties of the medium that generates them. The various kinds of nonlinear spectroscopy fall into the second category. Saturation spectroscopy deals typically with the . absorption of waves passing through a medium to be studied. In the simpl作者: 欲望小妹 時(shí)間: 2025-3-23 17:44
Managing the International R-to-D Interfacergies, e.g., in the third-order product .*.. This is built into the concept of the rotating-wave approximation, whether taken classically or quantum mechanically. Because of the .*, it is possible to conjugate a wave front. Section 2–4 discusses the conjugation of a plane wave front in a classical .作者: –吃 時(shí)間: 2025-3-23 20:14
Directors of International R&D Labs is a simple and useful example of multimode phenomena that can produce time variations in the laser. The present chapter considers a number of time-varying laser processes such as the relaxation oscillations in the ruby or semiconductor laser output, the build-up of multimode operation in lasers, t作者: 產(chǎn)生 時(shí)間: 2025-3-24 01:26 作者: IRATE 時(shí)間: 2025-3-24 05:33 作者: PON 時(shí)間: 2025-3-24 09:02
Fernando Perez-Ruiz,Ana Maria Herrero-Beites with many experiments. Nevertheless several significant experiments show strong disagreements with such semiclassical theories. The present Chapter treats the atom-field interaction fully quantum mechanically, providing a basic understanding of spontaneous emission and laying the foundations for th作者: Neuropeptides 時(shí)間: 2025-3-24 14:09 作者: accordance 時(shí)間: 2025-3-24 18:11
Getting TPAs to Act on a Projectontaneous emission of an atom irradiated by a continuous, monochromatic field. This emission is called .. We compute its spectrum, which is given in steady state by the Fourier transform of the first-order correlation function of the field. We also discuss the phenomenon of photon antibunching, a pu作者: 疏忽 時(shí)間: 2025-3-24 21:19
Public Consultation — Getting it Righty for Δ., has a built-in degree of freedom: one can squeeze the standard deviation of one observable provided one “stretches” that for the conjugate observable. For example the position and momentum standard deviations obey the uncertainty relation. and we can squeeze Δ. to an arbitrarily small valu作者: rectum 時(shí)間: 2025-3-24 23:24
Pathophysiology of Heart Failure2–14. So far, our treatment of quantized field-matter interactions has concentrated mostly on situations where the quantized field acts as a noise source: under these conditions the nonlinear atomic response originates from a . driving field, while the effects of the quantized modes are treated line作者: 喃喃訴苦 時(shí)間: 2025-3-25 05:12 作者: CHOP 時(shí)間: 2025-3-25 10:02
e a broad coverage of the basic elements that we consider necessary to carry out research in quantum optics. We have attempted to present a vari- ety of theoretical tools, so that after completion of the course students should be able to understand specialized research literature and to produce original resea978-3-662-11654-8作者: 煩人 時(shí)間: 2025-3-25 14:05 作者: Coterminous 時(shí)間: 2025-3-25 16:33 作者: HATCH 時(shí)間: 2025-3-25 23:16
Managing the International R-to-D Interfacees, the wave front would be inverted and sent back through the distorting medium to converge on the original point source. Such a phenomenon has been demonstrated using nonlinear optics and is of substantial interest in applications in laser fusion, weapons, and compensation for bad optics in genera作者: Flu表流動(dòng) 時(shí)間: 2025-3-26 00:26
Directors of International R&D Labst with different atoms, such as in a Doppler-broadened gaseous medium. While these can also be thought of as optical instabilities, we prefer to refer to them in the traditional way simply as multimode operation. In particular, this kind of operation can produce a periodic train of short pulses.作者: 一個(gè)姐姐 時(shí)間: 2025-3-26 05:28 作者: incite 時(shí)間: 2025-3-26 09:13
Classical Electromagnetic Fields,ssical description of light and a quantum mechanical description of matter is called the . approximation. This approximation is not always justified (see Chaps. 12 through 18), but there are remarkably few cases in quantum optics where we need to quantize the field.作者: 等待 時(shí)間: 2025-3-26 13:41
Introduction to Laser Theory,bsorption. This nonlinear cavity problem can lead to two or more stable output intensities for a given input intensity, and hence belongs to a class of problems called .. In the present chapter we also see a bistable configuration that involves active media, namely the homogeneously broadened ring l作者: commune 時(shí)間: 2025-3-26 17:00
Three and Four Wave Mixing,es, the wave front would be inverted and sent back through the distorting medium to converge on the original point source. Such a phenomenon has been demonstrated using nonlinear optics and is of substantial interest in applications in laser fusion, weapons, and compensation for bad optics in genera作者: 憤怒事實(shí) 時(shí)間: 2025-3-26 21:38
Time-Varying Phenomena in Cavities,t with different atoms, such as in a Doppler-broadened gaseous medium. While these can also be thought of as optical instabilities, we prefer to refer to them in the traditional way simply as multimode operation. In particular, this kind of operation can produce a periodic train of short pulses.作者: antiandrogen 時(shí)間: 2025-3-27 01:30
Coherent Transients,categorized as “coherent transients.” As the induced polarization decays due to various line broadening mechanisms, the coherent response is lost. The time taken for this decay is typically directly related to the dipole (..) and population (... decay times as well as to the width of the inhomogeneo作者: Inculcate 時(shí)間: 2025-3-27 08:26 作者: CLAIM 時(shí)間: 2025-3-27 12:06
Classical Nonlinear Optics,tion becomes too large for the medium to continue to respond linearly. We have already seen how a nonlinearity plays an essential role in the free electron laser pendulum equation (1.131). In another example that we discuss in detail in Chap. 6, the output intensity of a laser oscillator builds up u作者: 正式通知 時(shí)間: 2025-3-27 16:42
Quantum Mechanical Background,when this approach is justified and what to do when it isn’t. Unexcited systems interacting with radiation far from the system resonances can often be treated purely classically. The response of systems near and at resonance often deviates substantially from the classical descriptions. Since the las作者: 新義 時(shí)間: 2025-3-27 18:52 作者: AORTA 時(shí)間: 2025-3-28 00:33
CW Field Interactions,The density matrix is extended in a form known as the ., which treats collections of atomic responses simply. Section 5-1 deals with homogeneously-broadened media, while Sec. 5-2 includes inhomogeneous broadening. The induced polarization is used as a source in the slowly-varying Maxwell equations t作者: Dealing 時(shí)間: 2025-3-28 03:57
Introduction to Laser Theory,interaction of radiation with two-level atoms. We consider arrangements of two or three highly reflecting mirrors that form cavities as shown in Fig. 6-1. Light in these cavities leaks out (decays to its 1/. value) in a time ./. where . is the frequency of the light and . is the cavity quality facto作者: Spinous-Process 時(shí)間: 2025-3-28 09:56
Optical Bistability,output frequencies, imposed by the self-consistent laser equations, are compromises between the atomic and cavity natural frequencies. In this chapter, we discuss another situation involving a nonlinear medium in Fabry-Perot and ring cavities, but with two major changes: 1) the cavity output depends作者: constitutional 時(shí)間: 2025-3-28 13:16
Saturation Spectroscopy,ility, etc. Alternatively one can use them to study the properties of the medium that generates them. The various kinds of nonlinear spectroscopy fall into the second category. Saturation spectroscopy deals typically with the . absorption of waves passing through a medium to be studied. In the simpl作者: ACTIN 時(shí)間: 2025-3-28 16:35
Three and Four Wave Mixing,rgies, e.g., in the third-order product .*.. This is built into the concept of the rotating-wave approximation, whether taken classically or quantum mechanically. Because of the .*, it is possible to conjugate a wave front. Section 2–4 discusses the conjugation of a plane wave front in a classical .作者: 一美元 時(shí)間: 2025-3-28 21:23 作者: 小蟲(chóng) 時(shí)間: 2025-3-29 00:39 作者: 上漲 時(shí)間: 2025-3-29 03:22
Field Quantization, to quantize the electromagnetic field. Such a semiclassical description is sufficient to describe most problems in quantum optics. However, there are a few notable exceptions where a classical description of the field leads to the wrong answer. These include spontaneous emission, the Lamb shift, re作者: 消散 時(shí)間: 2025-3-29 09:49
Interaction between Atoms and Quantized Fields, with many experiments. Nevertheless several significant experiments show strong disagreements with such semiclassical theories. The present Chapter treats the atom-field interaction fully quantum mechanically, providing a basic understanding of spontaneous emission and laying the foundations for th作者: atopic-rhinitis 時(shí)間: 2025-3-29 13:28
System-Reservoir Interactions,to a large system. In that case the small system is the atom and the large system is the continuum of modes of the electromagnetic field. When computing the atomic decay rate, we were not interested in the field itself, but only on its effect on the atomic dynamics. Thus we never explicitly computed作者: carotenoids 時(shí)間: 2025-3-29 17:54 作者: Blood-Clot 時(shí)間: 2025-3-29 22:56 作者: EVICT 時(shí)間: 2025-3-30 02:48
Quantum Theory of a Laser,2–14. So far, our treatment of quantized field-matter interactions has concentrated mostly on situations where the quantized field acts as a noise source: under these conditions the nonlinear atomic response originates from a . driving field, while the effects of the quantized modes are treated line作者: 進(jìn)步 時(shí)間: 2025-3-30 06:21 作者: CHANT 時(shí)間: 2025-3-30 08:26
CW Field Interactions,o yield a nonlinear Beer’s law for propagation. The population matrix equations of motion are solved in the important ., which assumes that the dipole lifetime .. is short compared to times for which the field envelope or population difference vary appreciably. The concepts of power-broadening and spectral hole burning are developed.作者: abreast 時(shí)間: 2025-3-30 14:23
Saturation Spectroscopy,est case, . acts alone and one studies the probe absorption as a function of the intensity. The formulas for this are given earlier in Sec. 5-1, since this problem is of substantial use not only in spectroscopy, but also in laser theory and optical bistability.作者: BANAL 時(shí)間: 2025-3-30 20:26 作者: idiopathic 時(shí)間: 2025-3-30 20:57 作者: Finasteride 時(shí)間: 2025-3-31 01:34
Quantum Theory of a Laser,rce: under these conditions the nonlinear atomic response originates from a . driving field, while the effects of the quantized modes are treated linearly. A notable exception was the Jaynes-Cummings model, where the Hamiltonian can be diagonalized exactly and hence the quantized mode is treated to all orders.作者: Nucleate 時(shí)間: 2025-3-31 06:40
Esophageal Disease in Diabetes Mellitus,o yield a nonlinear Beer’s law for propagation. The population matrix equations of motion are solved in the important ., which assumes that the dipole lifetime .. is short compared to times for which the field envelope or population difference vary appreciably. The concepts of power-broadening and spectral hole burning are developed.作者: 禁止,切斷 時(shí)間: 2025-3-31 11:00
Schering: Synchronised Drug Developmentest case, . acts alone and one studies the probe absorption as a function of the intensity. The formulas for this are given earlier in Sec. 5-1, since this problem is of substantial use not only in spectroscopy, but also in laser theory and optical bistability.
